<p>We generalize some fundamental results for noncompact Riemannian manfolds without boundary, that only require completeness and no curvature assumptions, to manifolds with boundary: let <i>M</i> be a smooth Riemannian manifold with boundary <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_1972_Article_IEq1.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="31" /> </InlineMediaObject> <EquationSource Format="TEX">\(\partial M\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>∂</mi> <mi>M</mi> </mrow> </math></EquationSource> </InlineEquation> and let <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_1972_Article_IEq2.gif" Format="GIF" Height="23" Rendition="HTML" Resolution="72" Type="Linedraw" Width="58" /> </InlineMediaObject> <EquationSource Format="TEX">\(\hat{C}^\infty _c(M)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msubsup> <mover accent="true"> <mi>C</mi> <mo stretchy="false">^</mo> </mover> <mi>c</mi> <mi>∞</mi> </msubsup> <mrow> <mo stretchy="false">(</mo> <mi>M</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> denote the space of smooth compactly supported cut-off functions with vanishing normal derivative, <i>Neumann cut-offs</i>. We show, among other things, that under completeness:<UnorderedList Mark="Bullet"> <ItemContent> <p><InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_1972_Article_IEq3.gif" Format="GIF" Height="23" Rendition="HTML" Resolution="72" Type="Linedraw" Width="58" /> </InlineMediaObject> <EquationSource Format="TEX">\(\hat{C}^\infty _c(M)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msubsup> <mover accent="true"> <mi>C</mi> <mo stretchy="false">^</mo> </mover> <mi>c</mi> <mi>∞</mi> </msubsup> <mrow> <mo stretchy="false">(</mo> <mi>M</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> is dense in <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_1972_Article_IEq4.gif" Format="GIF" Height="23" Rendition="HTML" Resolution="72" Type="Linedraw" Width="66" /> </InlineMediaObject> <EquationSource Format="TEX">\(W^{1,p}(\mathring{M})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>W</mi> <mrow> <mn>1</mn> <mo>,</mo> <mi>p</mi> </mrow> </msup> <mrow> <mo stretchy="false">(</mo> <mover accent="true"> <mi>M</mi> <mo>˚</mo> </mover> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> for all <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_1972_Article_IEq5.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="77" /> </InlineMediaObject> <EquationSource Format="TEX">\(p\in (1,\infty )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>p</mi> <mo>∈</mo> <mo stretchy="false">(</mo> <mn>1</mn> <mo>,</mo> <mi>∞</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation>; this generalizes a classical result by Aubin (Bull. Sci. Math. 100:149–173, 1976) for <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_1972_Article_IEq6.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="63" /> </InlineMediaObject> <EquationSource Format="TEX">\(\partial M=\emptyset \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>∂</mi> <mi>M</mi> <mo>=</mo> <mi mathvariant="normal">∅</mi> </mrow> </math></EquationSource> </InlineEquation>.</p> </ItemContent> <ItemContent> <p><i>M</i> admits a sequence of first order cut-off functions in <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_1972_Article_IEq7.gif" Format="GIF" Height="23" Rendition="HTML" Resolution="72" Type="Linedraw" Width="58" /> </InlineMediaObject> <EquationSource Format="TEX">\(\hat{C}^\infty _c(M)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msubsup> <mover accent="true"> <mi>C</mi> <mo stretchy="false">^</mo> </mover> <mi>c</mi> <mi>∞</mi> </msubsup> <mrow> <mo stretchy="false">(</mo> <mi>M</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>; for <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_1972_Article_IEq8.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="63" /> </InlineMediaObject> <EquationSource Format="TEX">\(\partial M=\emptyset \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>∂</mi> <mi>M</mi> <mo>=</mo> <mi mathvariant="normal">∅</mi> </mrow> </math></EquationSource> </InlineEquation> this result can be traced back to Gaffney (Ann. Math. (2) 60(1):140–145, 1954).</p> </ItemContent> <ItemContent> <p>the Laplace–Beltrami operator with domain of definition <InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_1972_Article_IEq9.gif" Format="GIF" Height="23" Rendition="HTML" Resolution="72" Type="Linedraw" Width="58" /> </InlineMediaObject> <EquationSource Format="TEX">\(\hat{C}^\infty _c(M)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msubsup> <mover accent="true"> <mi>C</mi> <mo stretchy="false">^</mo> </mover> <mi>c</mi> <mi>∞</mi> </msubsup> <mrow> <mo stretchy="false">(</mo> <mi>M</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> is essentially self-adjoint; this is a generalization of a classical result by Strichartz (J. Funct. Anal. 52(1):48–79, 1983) for <InlineEquation ID="IEq10"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_1972_Article_IEq10.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="63" /> </InlineMediaObject> <EquationSource Format="TEX">\(\partial M=\emptyset \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>∂</mi> <mi>M</mi> <mo>=</mo> <mi mathvariant="normal">∅</mi> </mrow> </math></EquationSource> </InlineEquation>.</p> </ItemContent> </UnorderedList></p>

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Neumann Cut-Offs and Essential Self-adjointness on Complete Riemannian Manifolds with Boundary

  • Davide Bianchi,
  • Batu Güneysu,
  • Alberto G. Setti

摘要

We generalize some fundamental results for noncompact Riemannian manfolds without boundary, that only require completeness and no curvature assumptions, to manifolds with boundary: let M be a smooth Riemannian manifold with boundary \(\partial M\) M and let \(\hat{C}^\infty _c(M)\) C ^ c ( M ) denote the space of smooth compactly supported cut-off functions with vanishing normal derivative, Neumann cut-offs. We show, among other things, that under completeness:

\(\hat{C}^\infty _c(M)\) C ^ c ( M ) is dense in \(W^{1,p}(\mathring{M})\) W 1 , p ( M ˚ ) for all \(p\in (1,\infty )\) p ( 1 , ) ; this generalizes a classical result by Aubin (Bull. Sci. Math. 100:149–173, 1976) for \(\partial M=\emptyset \) M = .

M admits a sequence of first order cut-off functions in \(\hat{C}^\infty _c(M)\) C ^ c ( M ) ; for \(\partial M=\emptyset \) M = this result can be traced back to Gaffney (Ann. Math. (2) 60(1):140–145, 1954).

the Laplace–Beltrami operator with domain of definition \(\hat{C}^\infty _c(M)\) C ^ c ( M ) is essentially self-adjoint; this is a generalization of a classical result by Strichartz (J. Funct. Anal. 52(1):48–79, 1983) for \(\partial M=\emptyset \) M = .